In this section, we incorporate the short-range correlations (SRCs) induced high momentum tail (HMT) into the calculations of the kinetic EOS of ANM in a space of general dimension \(d\) .
Here we first describe briefly the single-nucleon momentum distribution function \(n_{\mathbf {k}}^J\)  in ANM in 3D.
Based on predictions of microscopic nuclear many-body theories and relevant experimental
findings [1]}, [2]}, [3]}, [4]}, the single-nucleon momentum distribution in ANM can be parametrized as [5]}, [6]}, [7]}, [8]},
\(n^J_{\mathbf {k}}(\rho ,\delta )=\left\lbrace \begin{array}{ll}\Delta _J,~~&0<|\mathbf {k}|<k_{\mathrm {F}}^J,\\\displaystyle {C}_J\left({k_{\mathrm {F}}^{J}}/{|\mathbf {k}|}\right)^4,~~&k_{\mathrm {F}}^J<|\mathbf {k}|<\phi _Jk_{\mathrm {F}}^J.\end{array}\right.\) 
